In theoretical physics, an M2-brane, is a spatially extended mathematical object that appears in string theory and in related theories (e.g. M-theory, F-theory). In particular, it is a solution of eleven-dimensional supergravity which possesses a three-dimensional world volume.
The M2-brane solution can be found by requiring                     (        P        o        i        n        c        a        r        e                  )                      3                          ×        S        O        (        8        )                 symmetry of the solution and solving the supergravity equations of motion with the p-brane ansatz. The solution is given by a metric and three-form gauge field which, in isotropic coordinates, can be written as
                                                                        d                                  s                                      M                    2                                                        2                                                                                              =                                                      (                    1                    +                                                                  q                                                  r                                                      6                                                                                                                )                                                        −                                                                  2                        3                                                                                            d                                  x                                      μ                                                  d                                  x                                      ν                                                                    η                                      μ                    ν                                                  +                                                      (                    1                    +                                                                  q                                                  r                                                      6                                                                                                                )                                                                              1                      3                                                                      d                                  x                                      i                                                  d                                  x                                      j                                                                    δ                                      i                    j                                                                                                                        F                                      i                                          μ                                              1                                                                                    μ                                              2                                                                                    μ                                              3                                                                                                                                        =                                  ϵ                                                            μ                                              1                                                                                    μ                                              2                                                                                    μ                                              3                                                                                                              ∂                                      i                                                                                        (                    1                    +                                                                  q                                                  r                                                      6                                                                                                                )                                                        −                    1                                                  ,                                μ                =                1                ,                …                ,                3                                i                =                4                ,                …                ,                11                ,                                                            where                     η                 is the flat-space metric and the distinction has been made between world volume                               x                      μ                                   and transverse                               x                      i                                   coordinates. The constant                     q                 is proportional to the charge of the brane which is given by the integral of                     F                 over the boundary of the transverse space of the brane.